Put . Retaining terms linear in gives
The exponential ansatz gives the characteristic equation of a delay differential equation
At its root is , and the remaining delay roots lie far in the left half-plane, so the equilibrium is stable for sufficiently small .
A stability change can first occur when . Separating real and imaginary parts gives
For the first positive crossing, and . Thus
All positive-frequency crossings have , so there is no earlier imaginary-axis crossing. Implicit differentiation of
gives, with ,
so the conjugate pair crosses into the right half-plane as increases. Therefore the stability threshold for delayed quadratic crowding is
Again put . Then
The linearized equation is therefore
whose sole characteristic exponent is and is independent of . By delay-independent stability from an undelayed linearization,

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